via \(A_H \rightarrow VV\)  to SM gauge bosons, which add extra jets and leptons
to the final state selection, but in most cases leaves enough missing
energy by a sufficient number of neutrinos. We used
MG5_aMC@NLO [1]} and
WHIZARD [2]} for the event generation,
PYTHIA8 [3]} for parton showering and
hadronization and Delphes [4]} for
detector simulation. The recasting of the SUSY searches from ATLAS and
CMS has been done with CheckMate [5]}. For more
details on the used analyses cf. [6]}.
<FIGURE>